1995A&A...297L..41V


Query : 1995A&A...297L..41V

1995A&A...297L..41V - Astronomy and Astrophysics, volume 297L41-44 (1995/5-2)

The magnetic field strength versus orbital period relation for binary radio pulsars with low-mass companions: evidence for neutron-star formation by accretion-induced collapse?

VAN DEN HEUVEL E.P.J. and BITZARAKI O.

Abstract (from CDS):

The 24 binary radio pulsars with nearly circular orbits and low-mass companions (0.2-0.4xM☉ helium white dwarfs in most cases) show a remarkable correlation between spin period P and orbital period Por and between dipole surface magnetic field strength BS, and Por. The observed BS, vs. Por relation is consistent with increasing decay of the neutron-star magnetic field with increasing amounts of matter accreted, as has been proposed on theoretical grounds by various authors. Neutron stars in binaries to which more than 0.45xfxM☉ was transferred have field strengths below 109G, where f(=<1) is the fraction of the transferred matter that is not lost from the systems. The only one exception in the galactic disk (out of twelve systems) is the PSR 1831-00 system, in which >0.7xfxM☉ was transferred but the pulsar still has a strong magnetic field (∼0.8x1011G). Adopting the field decay by accretion models, the only way in which this can be explained is that the neutron star in this system was formed near the end of the mass-transfer phase, by the accretion-induced collapse (AIC) of a white dwarf.

Abstract Copyright: ∼

Journal keyword(s): neutron stars - binary pulsars - pulsars - accretion-induced collapse

Simbad objects: 26

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Number of rows : 26
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 PSR J0023-7203J Psr 00 23 59.40735 -72 03 58.7914           ~ 91 1
2 PSR B0021-72I Psr 00 24 07.9330 -72 04 39.669           ~ 68 1
3 PSR J0024-7204E Psr 00 24 11.125 -72 05 20.14           ~ 66 1
4 PSR J0034-05 Psr 00 34 21.8281 -05 34 36.620           ~ 201 0
5 PSR J0218+42 Psr 02 18 06.3604 +42 32 17.365           ~ 365 2
6 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
7 PSR J0823+0159 Psr 08 23 09.78731 +01 59 12.6003           DA 244 0
8 PSR J1045-45 Psr 10 45 50.179671 -45 09 54.05686           ~ 154 1
9 PSR J1312+1810 Psr 13 12 55 +18 10.0           ~ 44 1
10 PSR B1620-26 Psr 16 23 38.2218 -26 31 53.769     21.30     ~ 318 2
11 PSR J1641+3627B Psr 16 41 41.0 +36 27 37           ~ 29 1
12 V* HZ Her LXB 16 57 49.8110126616 +35 20 32.486555472 11.90 14.89 13.63 13.88   B3/6ep 2172 0
13 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
14 PSR B1718-19 Psr 17 21 01.48 -19 36 51.0           ~ 97 1
15 NGC 6342 GlC 17 21 10.14 -19 35 14.7     10.01     ~ 310 0
16 PSR B1744-24A Psr 17 48 02.249 -24 46 37.65           ~ 235 0
17 PSR B1800-27 Psr 18 03 31.692 -27 12 06.00           ~ 57 0
18 PSR B1831-00 Psr 18 34 17.25 -00 10 53.3           DA 101 0
19 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
20 PSR B1908+00A Psr 19 11 11.02 +01 02 10.9           ~ 51 0
21 PSR B1953+29 Psr 19 55 27.8680959374 +29 08 43.499227152           ~ 303 1
22 PSR J1959+2048 Psr 19 59 36.7643141520 +20 48 14.896407996   21.08 20.16 19.53 18.79 G: 854 3
23 PSR J2019+24 Psr 20 19 31.94900 +24 25 15.3038           ~ 145 1
24 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0
25 PSR J2229+26 Psr 22 29 50.883815 +26 43 57.61393           ~ 121 1
26 PSR J2317+1439 Psr 23 17 09.235606 +14 39 31.29559           ~ 211 1

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